Reflectance measurements of layered media with diffuse photon-density waves: a potential tool for evaluating deep burns and subcutaneous lesions.

The basic principles of a non-contact, near-infrared technique for the mapping of layered tissues are discussed theoretically and verified experimentally. The propagation properties of diffuse photon-density waves in tissues depend on the optical properties of the tissue. When a layered medium is irradiated by amplitude modulated light, the difference in optical properties between the layers is evident in the phase and amplitude of the diffuse reflection coefficient, which is a result of the interference of the partial waves propagating in the different layers. Thus, diffuse photon-density waves are applicable to the analysis of the structure of layered tissue. The probing depth is determined by the modulation frequency of the incident light. For modulation frequencies between several hundred megahertz and a few gigahertz, this allows us to analyse the properties of muscle tissue of up to 4-8 mm below the surface. Experimental results based on chicken breast muscle are given. As an example, the technique might be of use for evaluating the depth of necrosis and the blood volume fraction in deep burns.

[1]  Lars O. Svaasand,et al.  Application of optical diffusion theory to transcutaneous bilirubinometry , 1998, European Conference on Biomedical Optics.

[2]  M. Patterson,et al.  Noninvasive determination of the optical properties of two-layered turbid media , 1998 .

[3]  Y Wang,et al.  Sensitivity studies for imaging a spherical object embedded in a spherically symmetric, two-layer turbid medium with photon-density waves. , 1996, Applied optics.

[4]  Bruce J. Tromberg,et al.  Tissue characterization and imaging using photon density waves , 1993 .

[5]  Enrico Gratton,et al.  Diffusion of intensity-modulated near-infrared light in turbid media , 1991, Photonics West - Lasers and Applications in Science and Engineering.

[6]  M. Patterson,et al.  Accuracy of the diffusion approximation in determining the optical properties of a two-layer turbid medium. , 1998, Applied optics.

[7]  Simon R. Arridge,et al.  Reconstruction methods for infrared absorption imaging , 1991, Photonics West - Lasers and Applications in Science and Engineering.

[8]  L V Wang,et al.  Anisotropy in the absorption and scattering spectra of chicken breast tissue. , 1998, Applied optics.

[9]  Bruce J. Tromberg,et al.  Reflectance tomography of two-layered turbid media with diffuse photon-density waves , 1998, European Conference on Biomedical Optics.

[10]  J. Haselgrove,et al.  Photon hitting density. , 1993, Applied optics.

[11]  N. N. Akhmediev,et al.  Boundary conditions for excitons in CdS , 1995, Other Conferences.

[12]  Britton Chance,et al.  Time-resolved spectroscopy and imaging , 1995, Photonics West.

[13]  Joseph M. Schmitt,et al.  MODEL OF OPTICAL COHERENCE TOMOGRAPHY OF HETEROGENEOUS TISSUE , 1997 .

[14]  J. Schmitt,et al.  Confocal microscopy in turbid media. , 1994, Journal of the Optical Society of America. A, Optics, image science, and vision.

[15]  Adolf Friedrich Fercher Optical coherence tomography. , 1996 .

[16]  B. Wilson,et al.  Time resolved reflectance and transmittance for the non-invasive measurement of tissue optical properties. , 1989, Applied optics.

[17]  Ashleyj . Welch,et al.  Optical-Thermal Response of Laser-Irradiated Tissue , 1995 .

[18]  L. O. Svaasand,et al.  Boundary conditions for the diffusion equation in radiative transfer. , 1994, Journal of the Optical Society of America. A, Optics, image science, and vision.

[19]  E R Anderson,et al.  Frequency-domain photon migration measurements of normal and malignant tissue optical properties in a human subject. , 1997, Applied optics.

[20]  Chance,et al.  Scattering and wavelength transduction of diffuse photon density waves. , 1993, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[21]  A. Welch,et al.  A review of the optical properties of biological tissues , 1990 .